Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Letters A

Critical assessment of the Schrödinger picture of quantum mechanics

A. J. de Faria, H. M. França, Coraci Pereira Malta, R. C. Sponchiado

Published Dec 1, 2002• 7 citations
Publisher
DOI
10.1016/s0375-9601(02)01508-6

Related papers

Comment on: “Critical assessment of the Schrödinger picture of quantum mechanics”

Hrvoje Nikolić

arXiv:quant-ph/0309136•Physics Letters A•Apr 24, 2004•1 citation

The Schrödinger Picture of Quantum Mechanics

Nima Moshayedi

SpringerBriefs in physics•Jan 1, 2023•0 citations

On the Formulation of Quantum Mechanics associated with Classical Pictures

Takehiko Takabayasi

By re-expressing the generalized Schrodinger equation in its coordinate representation in terms of amplitude and phase of the state vector, a quantum-mechanical change of a system can be made to correspond to an ensemble of classical motions of the system to which is added some internal potential. This ensemble may be taken as the statistical. This enables an alternative formulation of quantum mechanics with which is associated that classical picture. Such a formulation leads, however, if developed straightforwardly according to the picture, to a theoretical scheme quite different from that of ordinary quantum mechanics concerning the problems other than the equation of motion. Furthermore, this formulation is not applicable to Fermions when spin, or exclusion principle is taken into account. Bohm's recent renewed form of the statistical interpretation of quantum mechanics referring to this formulation is criticized in several points. On this formulation we can construct a singular ensemble which is shown to correspond to the transformation kernel of the wave function to infinitesimally later instant, and thus a connection between this formulation and that of Feynman's is taken out. Hydrodynamical picture formally equivalent to the statistical picture in one-body problems is also considered, and from such analogy certain formal generalization of Schrodinger equation is suggested.

Progress of Theoretical Physics•Aug 1, 1952•340 citations

Schrödinger and the interpretation of quantum mechanics

Fritz Rohrlich

Foundations of Physics•Dec 1, 1987•6 citations

Locality in the Schrödinger Picture of Quantum Mechanics

Vlatko Vedral

This paper explains how the so-called Einstein locality is to be understood in the Schrödinger picture of quantum mechanics. This notion is fully compatible with the Bell non-locality exhibited by entangled states. Contrary to the belief that quantum mechanics is incomplete, it is, As a matter of fact, its overcompleteness, as exemplified by the different pictures of quantum physics, that points to the same underlying reality.

Physics•May 19, 2024•1 citation

The Schrödinger Realization of Quantum Mechanics

Daniel R. Bes

Springer eBooks•Jan 1, 2004•0 citations
By re-expressing the generalized Schrodinger equation in its coordinate representation in terms of amplitude and phase of the state vector, a quantum-mechanical change of a system can be made to correspond to an ensemble of classical motions of the system to which is added some internal potential. This ensemble may be taken as the statistical. This enables an alternative formulation of quantum mechanics with which is associated that classical picture. Such a formulation leads, however, if developed straightforwardly according to the picture, to a theoretical scheme quite different from that of ordinary quantum mechanics concerning the problems other than the equation of motion. Furthermore, this formulation is not applicable to Fermions when spin, or exclusion principle is taken into account. Bohm's recent renewed form of the statistical interpretation of quantum mechanics referring to this formulation is criticized in several points. On this formulation we can construct a singular ensemble which is shown to correspond to the transformation kernel of the wave function to infinitesimally later instant, and thus a connection between this formulation and that of Feynman's is taken out. Hydrodynamical picture formally equivalent to the statistical picture in one-body problems is also considered, and from such analogy certain formal generalization of Schrodinger equation is suggested.